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The Weak Charge of the Proton and New Physics

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arxiv hep-ph/0302149 v1 pith:KWTILGDF submitted 2003-02-17 hep-ph hep-ex

The Weak Charge of the Proton and New Physics

classification hep-ph hep-ex
keywords correctionsphysicsprotonweakchargecontributionselectroweakenergy
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We address the physics implications of a precision determination of the weak charge of the proton, QWP, from a parity violating elastic electron proton scattering experiment to be performed at the Jefferson Laboratory. We present the Standard Model (SM) expression for QWP including one-loop radiative corrections, and discuss in detail the theoretical uncertainties and missing higher order QCD corrections. Owing to a fortuitous cancellation, the value of QWP is suppressed in the SM, making it a unique place to look for physics beyond the SM. Examples include extra neutral gauge bosons, supersymmetry, and leptoquarks. We argue that a QWP measurement will provide an important complement to both high energy collider experiments and other low energy electroweak measurements. The anticipated experimental precision requires the knowledge of the order alpha_s corrections to the pure electroweak box contributions. We compute these contributions for QWP, as well as for the weak charges of heavy elements as determined from atomic parity violation.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Relative enhancement of low-mass vector-boson exchange in higher waves matrix elements: parity non-conservation in hydrogen

    hep-ph 2026-07 conditional novelty 5.0

    A light Z' boson can mix hydrogen's 3p and 3d states with no Standard Model Z background, offering a potentially clean atomic probe of new physics.

  2. Parity Nonconservation in Hydrogen Induced by Low-Mass Vector-Boson Exchange

    hep-ph 2026-05 unverdicted novelty 5.0

    The ratio of low-mass Z' to SM Z contributions to PNC in hydrogen and deuterium is computed for arbitrary Z' mass, showing faster-than-1/Z² growth at low Z for both nuclear-spin-independent and dependent cases.